198
DOC. 4
KINETIC THEORY LECTURE NOTES
We
calculate this
integral
for the
argument
H
+
e.
In
place
of
every
dH1
we
have
dH1
[1
+
e
H]
" " " "
Hx
" "
H1
1
+
H
i
0'
=
+
e)TldH1
1
+
,
where
e
is
°°
smaller
a,
=
n{co(H),+co'(H1)-e}
n
1
+
n
(dH,)
1
IldH1
»
nco(H1)n(dHl)\l
+
eYJ{°^l+
1
oÄH,) H,
[p. 49]
The Electron
Theory
of
M[etals][93]
F
=
-
1
,dG
RT
dT
3
dz
ncA
uN
dz
ldfi
2
dT
3
RT
K
=
-
1
:
R
"n(c)Ac
/
\,
2
~W~!h
/iC2
=
~JiN~
2
HNv
k
-
=
T
C
_Je^
=
c
\l
2
-
T
=
mean
veloc.
=
2
\ic
1
R
K
=
-
nkc
2 liN
03^7=
d2
03FT.
l2
K
-
1
e2
nk
a
Ne5
2
fi
c I
3RT
HN